Patterned strained semiconductor substrate and device

ABSTRACT

A method that includes forming a pattern of strained material and relaxed material on a substrate; forming a strained device in the strained material; and forming a non-strained device in the relaxed material is disclosed. In one embodiment, the strained material is silicon (Si) in either a tensile or compressive state, and the relaxed material is Si in a normal state. A buffer layer of silicon germanium (SiGe), silicon carbon (SiC), or similar material is formed on the substrate and has a lattice constant/structure mis-match with the substrate. A relaxed layer of SiGe, SiC, or similar material is formed on the buffer layer and places the strained material in the tensile or compressive state. In another embodiment, carbon-doped silicon or germanium-doped silicon is used to form the strained material. The structure includes a multi-layered substrate having strained and non-strained materials patterned thereon.

BACKGROUND OF INVENTION

The invention relates to methods and structures for manufacturing semiconductor devices having improved device performances, and more particularly, to methods and structures for forming patterns of strained and non-strained areas on a substrate.

Emerging technologies, such as embedded Dynamic Random Access Memory (eDRAM), Application Specific Integrated Circuits (ASIC), and system-on-chip (SoC), require the combination of high-performance logic devices and memory devices on the same chip. It is also desired to have digital circuits and analog circuits on the same chip for some applications. It has been shown that logic devices exhibit better performance when formed on a tensily strained silicon layer that is epitaxially grown on another epitaxially grown silicon germanium (SiGe) layer that has been relaxed.

A fully relaxed SiGe layer has a lattice constant which is larger than that of silicon. Thus, when the silicon layer is epitaxially grown thereon, the silicon layer conforms to the larger lattice constant of the relaxed SiGe layer and this applies physical biaxial stress to the silicon layer being formed thereon. This physical biaxial stress applied to the silicon layer increases the performance of logic devices formed in the strained silicon.

Relaxation in SiGe on silicon substrates occurs through the formation of misfit dislocations, which when equally spaced to relieve stress cause the substrate to be perfectly relaxed. Additionally, the misfit dislocations provide extra half-planes of silicon in the substrate. This allows the lattice constant in the SiGe layer to seek its intrinsic value. In this manner, the SiGe lattice constant grows larger as the mismatch strain across the SiGe/silicon interface is accommodated.

The problem with this approach is that it requires a very thick, multilayered SiGe layer. Additionally, the misfit dis-locations formed between the SiGe layer and the epitaxial silicon layer are random, highly non-uniform in density, and fairly uncontrollable due to heterogeneous nucleation that cannot be easily controlled. Consequently, the physical stress applied to the silicon layer is apt to be defective. At locations where misfit density is high, defects form in the strained silicon layer. These defects short device terminals and cause other leakage problems. For this reason, although the performance of logic devices is strengthened when the logic devices are formed in areas of strained silicon, the performance of defect-sensitive devices such as DRAM devices degrades when formed therein. The production yield is also compromised when the defect-sensitive devices are formed in the strained regions. Thus a need exists for a method of (and a substrate for) manufacturing strained and non-strained silicon regions on the same chip so that high-performance logic devices can be made in the strained silicon regions and high quality, defect-sensitive devices can be made in the non-strained regions.

SUMMARY OF INVENTION

In one aspect of the invention, a method for forming an electrical device is provided. The method includes forming a pattern of strained material and non-strained (relaxed) material on a substrate. The method further includes forming a strained device in the strained material. The method yet further includes forming a non-strained device in the non-strained material.

In another aspect of the invention, another method for forming an electrical device is provided. The method includes forming a buffer layer in contact with a portion of a substrate. The buffer layer has a lattice constant/structure mismatch with the substrate. The method also includes forming a relaxed layer on the buffer layer. The method further includes forming a strained material on a top surface of the relaxed layer. The relaxed layer places the strained material in one of a tensile or a compressive state. The method yet further includes patterning a non-strained (relaxed) material proximate the strained material.

In still another aspect of the invention, an electrical device is provided. The device includes a substrate. The device further includes a pattern of strained material and relaxed material formed on the substrate. The device yet further includes a strained device formed in the strained material. The device still further includes a non-strained device formed in the relaxed material.

In yet another aspect of the invention, another electrical device is provided. The electrical device includes a buffer layer formed in contact with a portion of a substrate. The buffer layer has a lattice constant/structure mismatch with the substrate. The device further includes a relaxed layer formed on the buffer layer. The device also includes a strained material formed on a top surface of the relaxed layer. The relaxed layer places the strained material in one of a tensile or a compressive state. The device still further includes a non-strained material patterned proximate the strained material.

BRIEF DESCRIPTION OF DRAWINGS

FIGS. 1-4 show fabricating steps of manufacturing an electrical device according to a first embodiment of the invention;

FIG. 5 shows a final structure of an electrical device according to a first embodiment of the invention;

FIGS. 6-10 show fabricating steps of manufacturing an electrical device according to a second embodiment of the invention;

FIG. 11 shows a final structure of an electrical device according to a second embodiment of the invention;

FIGS. 12-15 show fabricating steps of manufacturing an electrical device according to a third embodiment of the invention;

FIG. 16 shows a final structure of an electrical device according to a third embodiment of the invention;

FIGS. 17-21 show fabricating steps of manufacturing an electrical device according to a fourth embodiment of the invention;

FIG. 22 shows a final structure of an electrical device according to a fourth embodiment of the invention;

FIGS. 23-26 show fabricating steps of manufacturing an electrical device according to a fifth embodiment of the invention;

FIG. 27 shows a final structure of an electrical device according to a fifth embodiment of the invention;

FIGS. 28-31 show fabricating steps of manufacturing an electrical device according to a sixth embodiment of the invention;

FIG. 32 shows a final structure of an electrical device according to a sixth embodiment of the invention;

FIG. 33 is a cross-sectional view of an electrical device according to a seventh embodiment of the invention that is formed using a combination of the methods and materials shown in FIGS. 1-32;

FIG. 34 is a flowchart representing fabricating steps of manufacturing the electrical device shown in FIGS. 1-5;

FIG. 35 is a flowchart representing fabricating steps of manufacturing the electrical device shown in FIGS. 6-11;

FIG. 36 is a flowchart representing fabricating steps of manufacturing the electrical device shown in FIGS. 12-16;

FIG. 37 is a flowchart representing fabricating steps of manufacturing the electrical device shown in FIGS. 17-22;

FIG. 38 is a flowchart representing fabricating steps of manufacturing the electrical device shown in FIGS. 23-27; and

FIG. 39 is a flowchart representing fabricating steps of manufacturing the electrical device shown in FIGS. 28-32.

DETAILED DESCRIPTION

The invention is directed to an electrical, digital, semiconductor, or other device having a substrate on which a pattern of strained and non-strained (i.e., relaxed) materials are formed. The strained material may be placed in tension or compression due to a lattice constant/structure difference with an underlying layer of relaxed material. In turn, the relaxed material is formed on a buffer layer, which contacts a portion of the substrate.

A material forming the buffer layer varies in concentration throughout the layer, and has a lattice constant/structure mismatch with the material that forms the substrate. Because the material forming the buffer layer increases in concentration the further the buffer layer extends from the substrate, defects normally caused by the lattice mis-match are virtually eliminated. The formation of the relaxed layer on the buffer layer further reduces and/or eliminates defects to such an extent that the strained material is virtually free of defects. The drastic reduction or elimination of defects in the strained material allows electronic or digital devices formed therein to operate very fast and very efficiently. It also allows devices such as Dynamic Random Access Memory (DRAM) to be formed in an adjacent relaxed material because such devices are normally very sensitive to defects. Thus, embodiments of the invention permit the forming of strained logic devices and non-strained memory devices side by side on the same substrate.

Referring now to FIGS. 1-5, there is shown a cross-section of a portion of an electrical device 100. “Electrical device”refers to an electrical, electro-mechanical, semiconductor, digital, or similar device. Illustrative types of electrical devices include, but are not limited to, transistors, capacitors, resistors, logic devices, memory devices, computer processors, traces, vias, semi-conductor wafer, computer chip, application specific integrated circuit (ASIC), system-on-chip (SoC), and the like. As shown in FIG. 1, the electrical device 100 includes a substrate 101 covered with a pad layer 103.

The substrate 101 is formed of any suitable material, for example, silicon (Si). Other suitable alternative types of substrates include germanium (Ge), silicon germanium (SiGe), silicon carbide (SiC), and those consisting essentially of one or more compound semiconductors having a composition defined by the formula Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1 (1 being the total relative mole quantity). Other suitable substrates have a composition Zn_(A1) Cd_(A2) Se_(B1) Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1 (1 being a total mole quantity). Alternatively, the substrate has a semiconductor-on-insulator type structure, e.g., a silicon-on-insulator (SOI) substrate. In one embodiment, the thickness of the substrate approximates that of a standard semiconductor wafer known in the art.

The pad layer 103 acts to prevent the layers which are directly beneath it from being removed by any of the subsequent processes. By selectively patterning openings in the pad layer, recesses can be formed through all or portions of the underlying substrate layers, as discussed below. Additionally, use of the pad layer permits the epitaxial growth (and deposition) of specific materials such as Si, Ge, SiGe, SiC, those consisting essentially of one or more compound semiconductors having a composition defined by the formula Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1 (1 being the total relative mole quantity), and those having a composition Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1 (1 being a total mole quantity). Each of these exemplary materials may be applied to all embodiments described herein.

The material forming the pad layer 103 will vary depending on the type of manufacturing process used. Exemplary pad layer materials include, but are not limited to, silicon nitride and/or silicon oxide. Persons skilled in the art, however, will readily understand additional types of materials that can be used to form the pad layer. Illustratively, the pad layer has an overall thickness of about 0.2 microns when it is desired to form a recess that is approximately 2.0 micron deep. This exemplary thickness may be applied to all embodiments herein described.

In FIG. 2, the substrate 101 is shown having a recess 105 formed therein formed using reactive ion etching or dry etching processes. The exact width of recess 105 is not critical, but the depth is formed in the range of about 1.0 micron to about 3.0 microns deep. An exemplary width is about 100 microns. These illustrative recess measurements may be applied to all embodiments disclosed herein. Thereafter, an insulating layer 107 formed of an oxide or nitride material is conformally deposited on the sidewalls and bottom 109 of the recess 105 using any suitable deposition or growth process known in the art. Illustratively, the insulating layer is formed to be in the range of approximately 10 Angstroms to about 100 Angstroms thick. This exemplary measurement may be applied to all embodiments described herein. After the insulating layer 107 is formed, lateral, but not vertical, portions thereof are removed from the recess using anisotropic etching such as reactive ion etching (RIE). That is, the portion of the insulating layer 107 formed on the recess bottom 109 is removed; however the insulating layer formed on the recess sidewalls remains thereon. The end result is that the recess bottom 109 is exposed while the recess sidewalls are conformally coated with the insulating layer 107. In this illustrative embodiment, the insulating layer 107 is also formed on the interior exposed edges of the pad layer, as shown.

In FIG. 3, a buffer layer 113 forms a lattice constant/structure mismatch 121 with the substrate 101 and functions to constrain most of the dislocations caused by the mismatch. Illustratively, the buffer layer may have an overall thickness from less than about 0.5 microns to more than about 2.0 microns. A relaxed layer 111 is formed on the buffer layer and remains relatively defect free. Illustratively, the overall thickness of the relaxed layer 111 may be about 0.2 microns. These exemplary thickness measurements may be applied to all the embodiments described herein.

The buffer layer 113 and the relaxed layer 111 are epitaxially grown in the recess 105, within the confines of the insulating layer 107. Buffer layer 113 is formed first, then the relaxed layer 111. The buffer layer 113 growth process starts from the recess bottom 109 and works upwards, layer after layer, until an overall thickness of approximately 0.5 micron to approximately 2.0 micron is reached. In one embodiment, silicon germanium (SiGe) is used to form the buffer layer 113 and the relaxed layer 111 in order to subsequently form a semiconductor layer such as silicon atop of the relaxed layer 111 with a tensile stress. In an alternative embodiment, silicon carbon (SiC) may be used to provide a compressive strain in the subsequently formed silicon layer.

The buffer layer 113 and the relaxed layer 111 may be deposited or grown using conventional techniques such as chemical vapor deposition methods. For example, ultrahigh vacuum chemical vapor deposition (UHVCVD) may be used in a conventional manner to grow a device quality SiGe or SiC layer. Other conventional techniques include rapid thermal chemical vapor deposition (RTCVD), lowpressure chemical vapor deposition (LPCVD), limited reaction processing CVD (LRPCVD) and molecular beam epitaxy (MBE). Optionally, a thin silicon buffer layer (not shown) may be formed on the interior walls of the recess 105 before SiGeor SiC formation.

The multi-layered buffer layer 113 is constructed in such a fashion that a concentration of a material (Ge, for example) incrementally increases from a base concentration 119 proximate the bottom of the recess to a benchmark concentration 117 proximate a top surface of the buffer layer. This incremental increase in concentration may be in any stepped fashion, such as for example, by 10% for each new deposition or grown layer. However, any percentage increase may be used depending on the desired applications and requested costs. In theory, the concentration of Ge can range from a base concentration of less than about 1% to a benchmark concentration of 100%. However, for cost and other reasons, a benchmark concentration of about 40% may be used. To prevent defects from occurring in the relaxed layer, the second base concentration 115 of a material used to form the relaxed layer 111 (i.e., Ge if SiGe is used) is chosen to approximately match the benchmark concentration 117 of Ge in the buffer layer 113.

Referring to FIG. 4, the pad layer is removed, and a layer of material (such as, but not limited to, Si) is epitaxially grown within and without the confines of the insulating layer 107 to formed relaxed material 123 and strained material 125. Material 123 is described as relaxed (or non-strained) because its lattice constant approximately equals the lattice constant of the substrate 101. Material 125 is described as strained because its lattice constant differs from the lattice constant of a material used to form the relaxed layer 111. Consequently, a lattice mismatch 127 occurs at the interface between the strained material 125 and the buffer layer 113. Depending on the type of material used to form the relaxed layer 111, strained material 125 may be placed in one of a tensile or a compressive state. Illustratively, strained material 125 is tensily strained when it is formed of Si and the relaxed layer is formed of SiGe. Alternatively, the strained material 125 is compressively strained when it is formed of Si and the relaxed layer 111 is formed of SiC. However, any two different semiconductor materials may be used, because the different lattice structure/constants of each material will exert either a compressive or tensile strain. In one embodiment, the strained material 125 and the relaxed material 123 each have an overall thickness from less than about 20 nanometers to more than about 100 nanometers. These exemplary thicknesses may be used in various embodiments herein described.

Referring to FIG. 5, a strained device 129 and a non-strained device 131 are formed in the strained material 125 and in relaxed material 123, respectively. Illustratively, strained material 129 is a logic device or a first transistor; and non-strained device 131 is DRAM or a second transistor.

Alternate embodiments and methods of manufacture will now be described with reference to FIGS. 6-11. Because the materials, etching methods, epitaxial growth methods, and deposition methods used to form the embodiments of FIGS. 6-11 are the same as those described above, these figures will be described in less detail in order not to unnecessarily obscure aspects of the invention.

In FIG. 6, a cross-section of an electrical device 100 is shown. The device 100 includes a substrate 101 covered by a pad layer 103. As shown in FIG. 7, a recess 105 is etched through the pad layer 103 and into the substrate 101 to a pre-determined depth, as described above. Thereafter, an oxide or nitride insulating layer 107 is conformally coated on the interior of the recess 105. The bottom portion of the insulating layer 107 is then removed, leaving the portions adhered to the recess sidewalls virtually intact.

FIG. 8 depicts the formation of the buffer layer 113 and the relaxed layer 111 in the recess 105, within the confines of the insulating layer 107. As mentioned above, a material forming the buffer layer varies in concentration from a base concentration 119 to a benchmark concentration 117. A second base concentration 115 of a material forming the relaxed layer 111 is chosen to approximately match the benchmark concentration 117 of the buffer layer 113. As previously disclosed, the buffer layer 113 functions to contain dislocations caused by the lattice mismatch 121. FIG. 9 illustrates the discrete and selective formation of a strained material 125 in the recess 105, within the confines of the insulating layer 107, and on top of the relaxed layer 111. As previously disclosed, the type of material used to form the relaxed layer 111 determines whether a tensile or compressive force is applied to the strained material 125.

FIG. 10 depicts removal of the pad layer 103 and subsequent planarization of the substrate 101. This Figure also illustrates the lattice mismatch 127 between the strained material 125 and the relaxed layer 111. The type of process used to remove the pad layer depends on the type of material used to form such layers. For example, if silicon nitride is used as the pad layer, then a wet etch using hot phosphoric (H₃PO₄) may be used. The type of planarization method used may be any suitable planarization technique. For example, in one embodiment, chemical mechanical polishing (CMP) may be used. In another embodiment, a high temperature reflow process with the presence of hydrogen may be used.

FIG. 11 shows the formation of electrical devices 129 and 131 in the strained material 125 and in the non-strained regions of the substrate 101. In this embodiment, portions of the substrate 101 that are outside the confines of the insulating layer 107 form the relaxed material 123 shown in FIG. 4. As previously described, strained device 129 may illustratively be, but is not limited to, a logic device or a first transistor; non-strained device 131 may illustratively be, but is not limited to, a DRAM or a second transistor.

A third embodiment is shown with respect to FIGS. 12 16. FIG. 12 illustrates a cross-sectional view of an electrical device 100 (i.e., a silicon wafer), which includes a substrate 101 on which are formed, in ascending order, buffer layer 113, relaxed layer 111, and strained material 125. This Figure also illustrates the lattice mismatch 121 formed between the substrate 101 and a lower surface of the buffer layer 113, and the lattice mismatch 127 formed between the relaxed layer 111 and the strained material 125. These layers can be grown or deposited in any known manner, with the buffer layer 113 having, in one embodiment, a higher concentration of material closest to the strained layer and gradually decreasing in concentration. This will eliminate or reduce formation of defects in the end product.

FIG. 13 depicts the formation of a recess 105 that extends through the pad layer 103, the strained material 125, the relaxed layer 111, and the buffer layer 113, but which has as its bottom a portion of the top surface of the substrate 101.

FIG. 14 depicts the formation of insulating layer 107 on the sidewalls of the recess 105. The insulating layer 107 is formed by deposition or growth process followed by an etching process, as previously described. FIG. 15 shows a relaxed material (for example, Si) which is selectively and epitaxially grown in the recess within the confines of the insulating material to completely fill the recess. Thereafter, the pad layer is removed, and the substrate is planarized such that the exposed surfaces of the strained material 125, insulating material, and relaxed material 123 are approximately level. In this embodiment, the strained material 125 is outside, while the relaxed material 123 is within the confines of the insulating material 107. That is, the relaxed material is formed within the recess.

Referring to FIG. 16, there is illustrated the formation of a strained device 129 in the strained material 125 and the formation of a non-strained device 131 in the relaxed material 123. As shown, strained device 129 is located outside the confines of the insulating material, and the non-strained device is located within those confines.

A fourth embodiment is shown with respect to FIGS. 17 22. A cross-sectional view of an electrical device 100 in accordance with the fourth embodiment is shown in FIG. 17. The device 100 includes a substrate 101 on which a buffer layer 113 of SiGe is formed. In an alternate embodiment, SiC can also be formed. A relaxed layer 111, also formed of SiGe (or alternatively SiC), covers the top surface of the buffer layer. The lattice mismatch 121 between the buffer layer and the silicon substrate 101 is in the illustrative range of 2% or less. This means that the lattice constant of the lowest SiGe buffer layer differs from the lattice constant of the silicon substrate by about 2% or less. This same percentage may also be applicable for any of the embodiments disclosed herein.

FIG. 18 illustrates the formation of a recess 105 that extends through the pad layer 103, through the relaxed layer 111, and through the buffer layer 113 to expose a top surface of the silicon substrate 101. FIG. 19 depicts the formation of an insulating layer 107 on the sidewalls of the recess 105 and the formation of the relaxed material 123 in the recess, as previously described. In FIG. 20, the pad layer has been removed, and the top surface of relaxed layer 111, insulating layer 107, and relaxed material l23 have been planarized. Thereafter, as shown in FIG. 21, a layer of silicon is epitaxially grown to cover the entire planarized surface.

The result of this process is that the lattice mismatch between the relaxed layer and the silicon layer places a tensile or compressive strain on the silicon, thereby creating strained material 125. Because the lattice mismatch between another portion of the silicon layer and the relaxed material 123 (Si) is negligible, a relaxed (non-strained material) 124 is created within the confines of the recess 105. Although, in this embodiment, the insulating layer 107 does not separate the strained material 125 from the second relaxed material 124, the lateral strain between the strained material 125 and non-strained materials 124 is minimal compared to the strain imposed by the strain imposed by the relaxed layer 111.

FIG. 22 illustrates the formation of a strained device 129 in the strained material 125, and the formation of a non-strained device 131 in the relaxed material 124. As previously disclosed, the strained device 129 may be a logic device, and the non-strained device may be a DRAM. However, other electrical devices, such as transistors and capacitors, may also be used.

FIGS. 23-27 are cross-sectional views of an electrical device 100 that illustrate the formation of a strained material 125 using doped silicon on a substrate 101. As shown in FIG. 23, a pad layer 103 is formed on a silicon substrate 101. Then, as illustrated by FIG. 24, a recess 105 is etched through the pad layer and into the substrate 101 to an exemplary depth of approximately 0.05 or 1 microns, as measured from a top surface of the substrate 101. Thereafter, an optional insulating layer 107, formed of an oxide or a nitride material, is formed on the sidewalls of and bottom of the recess 105 using chemical vapor deposition or other known processes. Following an etching process to remove the insulating layer 107 from the bottom portion of the recess 105, a strained material 125 is epitaxially grown in the recess within the confines of the insulating material 107 until a top surface of the strained material approximately matches a top surface of the substrate 101. The strained layer 125 has a thickness less than the so-called “critical thickness”. The critical thickness is defined as the maximum thickness of the strained layer below which virtually no defects are generated. Illustratively, the strained material 125 is carbon-doped silicon. However, other doped semiconductor materials may be used. For example, a compressive-strained layer may be formed by forming a germanium-doped silicon layer on silicon substrate.

FIG. 26 shows that the pad layer 103 has been etched away using either a dry or wet etch, as previously described, and that the top surface of the substrate 101 is planarized to be approximately level with the top surfaces of strained material 125, insulating layer 107 and the substrate 101. In this manner, strained material 125 is selectively formed in the recess 105 and separated from the non-strained areas 126 of the substrate 101 by the insulating layer 107. As shown in FIG. 27, a strained device 129, such as a logic device, is formed in the strained material 125; and a non-strained device 131 is formed in the non strained area 126 of the substrate 101.

FIGS. 28-32 are cross-sectional views of an electrical device 100 that illustrate another formation of a strained material 125 using doped silicon on a silicon substrate 101. In FIG. 28, a silicon substrate 101 is prepared for processing. In FIG. 29, a carbon-doped strained material 125 is epitaxially grown on a top surface of the substrate 101. The strained layer 125 has a thickness less than the so-called “critical thickness”. The critical thickness is defined as the maximum thick of the strained layer below which there is virtually no defects is generated. Illustratively, the strained material 125 is carbon-doped silicon. However, other doped semiconductor materials may be used. For example, a compressive-strained layer may be formed by forming a germanium-doped silicon layer on silicon substrate.

In FIG. 30, a patterned pad layer 103 is formed on the strained material 125. Areas of the non-strained silicon substrate are exposed by using an etching process to remove areas of strained doped material 125 that are not covered by the pad layer 103.

In FIG. 31, a non-strained (relaxed) material 123 is epitaxially grown on the exposed areas of the substrate 101 to approximately the same height of the strained layer 125 to form a substantially planar top surface. Epitaxially growing the non-strained material 123 is optional, since the strained material 125, in this embodiment, is very thin (e.g., less than about 100 nanometers). Thereafter, as shown in FIG. 32, the pad layer 103 is etched away and a strained device 129 is formed in the strained material 125. A non-strained device 131 is formed in the relaxed material 123. Alternatively, if a relaxed material 123 is not used, the non-strained device 131 is formed in a non-strained area of the substrate 101. Again, permitting the strained material 125 to contact the adjacent relaxed material 123 usually does not pose problems because the lateral strain experienced by both materials is significantly less than the strain created by the doped semiconductor material that forms the strained material 125. Illustratively, the strained material 125 is carbon-doped silicon. However, other doped semiconductor materials may be used. For example, a compressive-strained layer may be formed by forming a germanium-doped silicon layer on silicon substrate.

FIG. 33 is a cross-sectional view illustrating an electrical device 100 having tensile-strained, compressive-strained, and non-strained materials 123, 124, and 123, respectively. As shown, each of these materials is formed on a surface of a substrate 101 using any combination of the techniques discussed above. The lateral strain experienced at junctions 133 is minimal compared to the vertical strain exerted by the lattice mismatches 127A and 127B, respectively. Alternatively, these layers may also be separated by insulating materials. In one embodiment, the tensile strained material 125A is a carbon-doped silicon layer formed on silicon and the compressive strained material 125B is a germanium-doped silicon layer formed on silicon. Alternatively, the tensile strained material 125A is a silicon layer formed on the SiGe buffer layer(s) (not shown) and the compressive strained material 125B is a silicon layer formed on SiC buffer layer(s) (not shown). Although illustratively shown as a layer, the relaxed material 123 may also be a relaxed top surface of the substrate 101, as previously illustrated and described with reference to FIGS. 31 and 32. Although illustratively shown that these layers have the same thickness, their thicknesses may not necessary be the same.

It should be understood that FIGS. 1-33 can equally represent methods of manufacture. In any event, FIGS. 34-39 show various methods for manufacturing the apparatus according to various aspects of the invention. Although herein described with reference to sequential reference numerals, the steps of each method may be performed in any order. The removing of layers to form a recess, forming layers and other processes may be provided by any known method of fabrication. For example, illustrative manufacturing processes include, but are not limited to, chemical vapor deposition, ultra-high vacuum chemical vapor deposition, and reactive ion etching (RIE), electrolytic etching, plasma etching, dry etching, and the like. Ion etching is a process of removing unwanted material by selectively bombarding an area or areas of a solid or liquid substance with energetic ionized particles. Often used in the manufacture of microelectronics, plasma etching creates reactive species in a plasma and then uses the reactive species to selectively remove unwanted material.

FIG. 34 is a flowchart illustrating an exemplary method of manufacturing an electrical device 100, according to one embodiment of the invention. At step 3401, a recess is patterned and formed in a substrate covered by a pad layer. At step 3403, an insulating layer is optionally formed on the sidewalls and bottom of the recess. At step 3405, a portion of the insulating layer is removed from the bottom of the recess to expose a portion of the sub-strate. At step 3407, a buffer layer is formed in the recess within the confines of the insulating layer, the buffer layer having a lattice constant/structure mismatch with the substrate. At step 3409 the concentration of a material forming the buffer layer is increased as the buffer layer is formed from a base concentration to a benchmark concentration. At step 3411, a relaxed layer is formed on the buffer layer. At step 3413, the pad layer is stripped. At step 3415, a strained material is formed on the relaxed layer within the confines of the insulating layer, and a non-strained material is formed on a portion of the sub-strate outside the confines of the insulating layer. At step 3417 a strained device is formed in the strained material. At step 3419 a non-strained device is formed in the relaxed material. In one embodiment, a material forming the relaxed layer has a second base concentration proximate a bottom surface thereof that approximately equals the benchmark concentration proximate a top surface of the buffer layer.

FIG. 35 is a flowchart illustrating an exemplary method of manufacturing an electrical device 100, according to one embodiment of the invention. At step 3501 a recess is patterned and formed in a substrate covered by a pad layer. At step 3503 an insulating layer is formed on the sidewalls and bottom of the recess. At step 3505, a portion of the insulating layer is removed from the bottom of the recess to expose a portion of the substrate. At step 3507, a buffer layer is formed in the recess within the confines of the insulating layer, the buffer layer having a lattice constant/structure mismatch with the substrate. At step 3509, the concentration of a material forming the buffer layer is increased as the buffer layer is formed, from a base concentration to a benchmark concentration. At step 3511 a relaxed layer is formed on the buffer layer. At step 3513 a strained material is formed on the relaxed layer in the recess within the confines of the insulating layer. At step 3515, the pad layer is stripped. At step 3517 the substrate is planarized. At step 3519 a strained device is formed in the strained material. At step 3521 a non-strained device is formed in the relaxed material. In one embodiment, a material forming the relaxed layer has a second base concentration proximate a bottom surface thereof that approximately equals the benchmark concentration proximate a top surface of the buffer layer.

FIG. 36 is a flowchart illustrating an exemplary method of manufacturing an electrical device 100, according to one embodiment of the invention. At step 3601 a pad layer is formed on a strained material. At step 3603, a recess is patterned and formed through the strained material, through a relaxed layer previously formed proximate thereto, and through a buffer layer previously formed proximate to the relaxed layer and in contact with a sub-strate. At step 3605 an insulating layer is formed on the sidewalls and bottom of the recess. At step 3607 the insulating layer is removed from the bottom of the recess. At step 3609, a relaxed material is formed in the recess within the confines of the insulating material. At step 3611, the pad layer is stripped. At step 3613, the sub-strate is planarized. At step 3615, a strained device is formed in the strained material. At step 3617 a non-strained device is formed in the relaxed material.

FIG. 37 is a flowchart illustrating an exemplary method of manufacturing an electrical device 100, according to one embodiment of the invention. At step 3701 a pad layer is patterned and formed on a relaxed layer previously formed on a buffer layer, the buffer layer being previously formed on a substrate. At step 3703 a recess is formed through the relaxed layer and the buffer layer. At step 3705 an insulating layer is formed on the sidewalls and bottom of the recess. At step 3707 a portion of the insulating layer is removed from the bottom of the recess to expose a portion of the substrate. At step 3709 a relaxed material in the recess within the confines of the insulating material. At step 3711 the pad layer is stripped. At step 3713 the substrate is planarized. At step 3715 a strained material is formed on the relaxed layer outside the confines of the insulating layer. At step 3717, a relaxed material is formed in the recess within the confines of the insulating layer. At step 3719, a strained device is formed in the strained material. At step 3721, a non-strained device is formed in the relaxed material.

FIG. 38 is a flowchart illustrating an exemplary method of manufacturing an electrical device 100, according to one embodiment of the invention. At step 3801 a recess is patterned and formed in a substrate covered by a pad layer. At step 3803 an insulating layer is formed on the sidewalls and bottom of the recess. At step 3805 a portion of the insulating layer from the bottom of the recess to expose a portion of the substrate. At step 3807 a strained material is selectively and epitaxially grown in the recess within the confines of the insulating layer. At step 3809, the pad layer is stripped. At step 3811, a strained device is formed in the strained material. At step 3813 a non-strained device is formed in a relaxed area of the substrate outside the confines of the insulating layer. In this embodiment, the strained material may be a carbon-doped material, such as, but not limited to, carbon-doped silicon. Alternatively, the strained material may be a germanium-doped material, such as, not limited to, germanium-doped silicon.

FIG. 39 is a flowchart illustrating an exemplary method of manufacturing an electrical device 100, according to one embodiment of the invention. At step 3901 a strained material is formed on a substrate. At step 3903 a pad layer is formed on the strained material. At step 3905, selective areas of the strained material are removed to expose corresponding portions of the substrate. At step 3907 a relaxed material is optionally grown on the exposed substrate to approximately the same height as the strained layer. At step 3909 the pad layer is stripped. At step 3911 a strained device is formed in the strained material. At step 3913 a non-strained device is formed in the relaxed material. In this embodiment, the strained material may be a carbon-doped material, such as, but not limited to, carbon-doped silicon.

Although embodiments of the invention have been illustrated in FIGS. 1-22 as fusing SiGe to form a tensile-strained material 125, it will be appreciated that other materials, such as SiC, may be substituted for SiGe, where it is desired to form a compressive-strained material 125. Additionally, a tensile-strained material 125 may be formed by epitaxially growing carbon-doped silicon on a silicon substrate. Other materials such as gallium phosphorus, gallium arsenic and the like, may also be substituted for SiGe, depending on desired applications and requested costs. As herein described, an electrical device formed in accordance with an embodiment of the invention may have a non-strained (relaxed) material 123, 124, 126 patterned proximate a strained material 125, 125A and 125B, as illustratively shown and described with respect to FIGS. 4, 15, 21, 26, 31 and 33.

While some exemplary embodiments of this invention have been described in detail, those skilled in the art will recognize that there are many possible modifications and variations which may be made in these exemplary embodiments while yet retaining many of the novel features and advantages of the invention. 

1. A method, comprising: forming a pattern of strained material and relaxed material on a substrate; forming a strained device in the strained material; and forming a non-strained device in the relaxed material.
 2. The method of claim 1, wherein the step of forming a pattern of strained material and relaxed material on a substrate further comprises: forming a recess in the substrate, the recess having sidewalls; forming a buffer layer in the recess which has a lattice constant/structure mismatch with the substrate; forming a relaxed layer on the buffer layer; forming the strained material on the relaxed layer and the relaxed material on the substrate, wherein the relaxed layer has a lattice constant/structure mismatch with the strained material.
 3. The method of claim 2, further comprising forming an insulating layer on the sidewalls before forming the buffer layer.
 4. The method of claim 2 wherein the relaxed layer and the buffer layer are each selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1 (1 being the total relative mole quantity), and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1 (1 being a total mole quantity).
 5. The method of claim 2, wherein the strained material and the relaxed material are each selected from one of the group consisting of silicon (Si), silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 6. The method of claim 2, wherein the step of forming the buffer layer further comprises: epitaxially growing multiple layers of a material forming the buffer layer such that the material forming the buffer layer has a base concentration proximate the substrate and an increased benchmark concentration proximate the relaxed layer.
 7. The method of claim 6, wherein the step of forming the relaxed layer further comprises: epitaxially growing multiple layers of a material forming the relaxed layer such that the material forming the relaxed layer has a second base concentration proximate the buffer layer that approximately equals the bench-mark concentration of the buffer layer material.
 8. The method of claim 1, wherein the step of forming the pattern of strained material and relaxed material on the substrate further comprises: forming a buffer layer on the substrate, the buffer layer having a lattice constant/structure mismatch with the substrate; forming a relaxed layer on the buffer layer; forming a recess through the relaxed layer and the buffer layer, the recess having sidewalls; forming the relaxed material in the recess; and forming the strained material on the relaxed layer outside the confines of the recess, the strained material having a lattice constant/structure mismatch with the relaxed layer.
 9. The method of claim 8, further comprises forming an insulating layer on the sidewalls before forming the relaxed layer in the recess.
 10. The method of claim 8, wherein the relaxed layer and the buffer layer are selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 11. The method of claim 8, wherein the step of forming the buffer layer further comprises epitaxially growing multiple layers of a material forming the buffer layer such that the material forming the buffer layer has a base concentration proximate the substrate and an increased bench-mark concentration proximate the relaxed layer.
 12. The method of claim 11, wherein the step of forming the relaxed layer further comprises epitaxially growing multiple layers of a material forming the relaxed layer such that the material forming the relaxed layer has a second base concentration proximate the buffer layer that approximately equals the benchmark concentration of the buffer layer material.
 13. The method of claim 1, wherein the strained material is formed of carbon-doped silicon or germanium doped silicon.
 14. A method for forming an electrical device, the method comprising: forming a buffer layer in contact with a portion of a sub-strate, the buffer layer having a lattice constant/structure mismatch with the substrate; forming a relaxed layer on the buffer layer; forming a strained material on a top surface of the relaxed layer, such that the relaxed layer places the strained material in one of a tensile or a compressive state; and patterning a non-strained material proximate the strained material.
 15. The method of claim 14, further comprising: forming a strained device in the strained material; and forming a non-strained device in the non-strained material.
 16. The method of claim 14, wherein the relaxed layer comprises a material which has a lattice constant/structure mismatch with the strained material.
 17. The method of claim 14, wherein the buffer layer is selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 18. The method of claim 14, wherein the step of forming the buffer layer further comprises epitaxially growing multiple layers of a material forming the buffer layer such that the material forming the buffer layer has a base concentration proximate the substrate and an increased bench-mark concentration proximate the relaxed layer.
 19. The method of claim 14, wherein the relaxed layer is selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 20. The method of claim 1, wherein the strained material is a semiconductor material doped by carbon or germanium.
 21. An electrical device, comprising: a pattern of strained material and relaxed material formed on a substrate; a buffer layer formed on the substrate and having a lattice constant/structure mismatch with the substrate; and a relaxed layer formed on the buffer layer, a top surface of the relaxed layer placing the strained material in one of a tensile or a compressive state, wherein the relaxed layer comprises a material which has a lattice constant/structure mismatch with the strained material, wherein a material forming the buffer layer increases in concentration from a base concentration proximate the substrate to a benchmark concentration proximate the relaxed layer.
 22. The electrical device of claim 21, further comprising a recess formed in the substrate and enclosing the buffer layer, the recess having sidewalls.
 23. The electrical device of claim 22, further comprising an insulating layer formed on the sidewalls.
 24. The electrical device of claim 21, wherein the relaxed layer and the buffer layer are selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 25. The electrical device of claim 21, wherein a material forming the relaxed layer has a second base concentration proximate the buffer layer that approximately equals the benchmark concentration.
 26. The electrical device of claim 23, wherein a material that forms the insulating layer is one of an oxide and a nitride.
 27. The electrical device of claim 23, wherein a portion of the substrate forms the relaxed material and is located outside a confine of the insulating material.
 28. The electrical device of claim 21, further comprising: a strained device formed in the strained material; and a non-strained device formed in the relaxed material.
 29. The electrical device of claim 23, wherein the relaxed material is formed in the recess within a confine of the insulating layer.
 30. The electrical device of claim 29, wherein the relaxed layer and the buffer layer are each selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb₄, where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 31. An electrical device, comprising: a pattern of strained material and relaxed material formed on a substrate; a first device formed in the first strained material; and a second device formed in the relaxed material.
 32. The electrical device of claim 31, further comprising: a buffer layer formed in contact with a portion of a sub-strate, the buffer layer having a lattice constant/structure mismatch with the substrate; a relaxed layer formed on the buffer layer; a strained material formed on a top surface of the relaxed layer, wherein the relaxed layer places the strained material in one of a tensile or a compressive state; and a non-strained material patterned proximate the strained material.
 33. The electrical device of claim 31, wherein the first device formed in the strained material is a logic device and the second device formed in the non-strained material is a defect-sensitive device.
 34. The electrical device of claim 32, wherein the relaxed material comprises a material which has a lattice constant/structure mismatch with the strained material.
 35. The electrical device of claim 32, wherein the buffer layer and the relaxed layer are selected from the group consisting of silicon carbon (SiC), silicon germanium (SiGe), Al_(X1)Ga_(X2)In_(X3)As_(Y1)P_(Y2)N_(Y3)Sb_(Y4), where X1, X2, X3, Y1, Y2, Y3, and Y4 represent relative proportions, each greater than or equal to zero and X1+X2+X3+Y1+Y2+Y3+Y4=1, and Zn_(A1)Cd_(A2)Se_(B1)Te_(B2), where A1, A2, B1, and B2 are relative proportions each greater than or equal to zero and A1+A2+B1+B2=1.
 36. The electrical device of claim 32, wherein a material forming the buffer layer increases in concentration from a base concentration proximate the substrate to a benchmark concentration proximate the relaxed layer.
 37. The electrical device of claim 32, wherein the strained material is a carbon doped semiconductor material or a germanium doped semiconductor material.
 38. The electrical device of claim 31, further comprising: a second strained material formed proximate the strained material and the non-strained material, wherein the strained material isaor compressive state and the second strained material is in a compressivetensile state, respectively.
 39. The electrical device of claim 31, wherein the strained material is a carbon doped material or a germanium doped material.
 40. The electrical device of claim 31, further comprising: a recess formed in the substrate, the recess having side-walls, wherein the strained material is formed within the confines of the sidewalls and is a carbon doped material or a germanium doped material.
 41. The electrical device of claim 40, wherein the sidewalls have an insulating layer and the strained material is formed within the confines of the insulating layer. 